English

Invariant holonomic systems on symmetric spaces and other polar representations

Representation Theory 2024-04-02 v2

Abstract

Let VV be a symmetric space over a connected reductive Lie algebra GG, with Lie algebra g\mathfrak{g} and discriminant δC[V]\delta\in \mathbb{C}[V]. A fundamental object is the invariant holonomic system G=D(V)/(D(V)g+D(V)(SymV)+G)\mathcal{G} =\mathcal{D}(V)\Big/ \Bigl(\mathcal{D}(V)\mathfrak{g}+ \mathcal{D}(V)(\mathrm{Sym}\, V)^G_+ \Bigr) over the ring of differential operators D(V)\mathcal{D}(V). Jointly with Levasseur we have shown that there exists a surjective radial parts map rad\mathrm{rad} from D(V)G \mathcal{D}(V)^G to the spherical subalgebra AκA_{\kappa} of a Cherednik algebra. When AκA_{\kappa} is simple we show that G\mathcal{G} has no δ\delta-torsion submodule nor factor module and we determine when G\mathcal{G} is semisimple, thereby answering questions of Sekiguchi, respectively Levasseur-Stafford. In the diagonal case when V=gV=\mathfrak{g}, these results reduce to fundamental theorems of Harish-Chandra and Hotta-Kashiwara. We generalise these results to polar representations VV satisfying natural conditions. By twisting the radial parts map, we obtain families of invariant holonomic systems. We introduce shift functors between the different twists. We show that the image of the simple summands of G\mathcal{G} under these functors is described by Opdam's KZ-twist.

Keywords

Cite

@article{arxiv.2109.11387,
  title  = {Invariant holonomic systems on symmetric spaces and other polar representations},
  author = {G. Bellamy and T. Nevins and J. T. Stafford},
  journal= {arXiv preprint arXiv:2109.11387},
  year   = {2024}
}

Comments

91 pages; typos corrected and references updated